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ElectricalElectromagnetics Field Theory
PrevNext

The charge density of a electrostatic field is

A

Curl(E)

B

Div(E)

C

Curl(D)

D

Div(D)

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalElectromagnetics Field Theory
Option D

Div(D)

Quick Summary:

According to Gauss's Law in differential form, the divergence of the electric flux density vector DтГЧ\vec{D}D is equal to the volume charge density ╧Бv\rho_v╧БvтАЛ at any given point in space. This relates the sources of the electrostatic field (charges) to the field itself.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

According to Gauss's Law in differential form, the divergence of the electric flux density vector DтГЧ\vec{D}D is equal to the volume charge density ╧Бv\rho_v╧БvтАЛ at any given point in space. This relates the sources of the electrostatic field (charges) to the field itself.

ЁЯФв Key Formulas

тИЗтЛЕDтГЧ=╧Бv\nabla \cdot \vec{D} = \rho_vтИЗтЛЕD=╧БvтАЛ тАФ Differential form of Gauss's Law

DтГЧ=╧╡0EтГЧ+PтГЧ\vec{D} = \epsilon_0 \vec{E} + \vec{P}D=╧╡0тАЛE+P тАФ Definition of electric flux density

тЪЩя╕П Working Principle

The operator тИЗтЛЕ\nabla \cdotтИЗтЛЕ (divergence) measures the outward flux density from an infinitesimal volume. Since DтГЧ=╧╡EтГЧ\vec{D} = \epsilon\vec{E}D=╧╡E, where ╧╡\epsilon╧╡ is the permittivity, the equation тИЗтЛЕDтГЧ=╧Бv\nabla \cdot \vec{D} = \rho_vтИЗтЛЕD=╧БvтАЛ implies that electric flux lines originate from positive charges and terminate on negative charges, quantifying the charge source density.

ЁЯУМ Key Points
  • тЦ╕

    Gauss's Law is one of Maxwell's four fundamental equations.

  • тЦ╕

    The SI unit for volume charge density ╧Бv\rho_v╧БvтАЛ is C/m3C/m^3C/m3.

  • тЦ╕

    Divergence represents the scalar source density of a vector field.

тЬЕ Advantages
  • тЦ╕

    Simplifies calculation of electric fields for symmetric charge distributions.

  • тЦ╕

    Provides a direct link between field sources and field intensity.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Limited to scenarios where symmetry can be exploited for easier integration.

  • тЦ╕

    Not sufficient to describe time-varying fields without Faraday's Law.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Calculating electric field intensity near conductors.

  • тЦ╕

    Determining capacitance of complex geometries.

  • тЦ╕

    Analyzing dielectric materials in capacitors.

ЁЯУД Additional Information
  • тЦ╕

    Option A (тИЗ├ЧEтГЧ=0\nabla \times \vec{E} = 0тИЗ├ЧE=0) characterizes the conservative nature of static electric fields.

  • тЦ╕

    Option B (тИЗтЛЕEтГЧ=╧Бv/╧╡0\nabla \cdot \vec{E} = \rho_v / \epsilon_0тИЗтЛЕE=╧БvтАЛ/╧╡0тАЛ) is an alternative form, but DтГЧ\vec{D}D is more fundamental when dealing with dielectric media.

  • тЦ╕

    Option C (тИЗ├ЧDтГЧ\nabla \times \vec{D}тИЗ├ЧD) is typically related to the existence of magnetic currents or time-varying magnetic fields (Maxwell-Ampere Law).

ЁЯУК Diagram / Illustration
Gauss Law FormulaтИЗ ┬╖ vec{D}╧Бс╡е
тЬЕ

D is correct тАФ The volume charge density ╧Бv\rho_v╧БvтАЛ is defined by the divergence of the electric flux density DтГЧ\vec{D}D, expressed as тИЗтЛЕDтГЧ=╧Бv\nabla \cdot \vec{D} = \rho_vтИЗтЛЕD=╧БvтАЛ.

Core Concepts Used
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Gauss's Law Divergence Operator Electric Flux Density
ЁЯТб EXAM TIP

Always remember that in electromagnetics, 'divergence' relates to sources (charges) while 'curl' relates to circulation or rotation (fields).

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